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Crystal Lattices and Unit Cells: Parameters & Packing

Crystal Lattices and Unit Cells: Parameters & Packing | chemca
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Physical Chemistry • The Solid State

Crystal Lattices and Unit Cells

Master the 3D geometry of solids, Bravais Lattices, and packing fractions.

By chemca Team • Updated Sep 2026

The rigid, beautiful, and highly anisotropic nature of crystalline solids stems entirely from their microscopic geometry. Atoms, ions, or molecules don't just clump together; they arrange themselves in perfect, mathematically repeating 3D patterns. To study the entire macroscopic crystal, we only need to study its smallest fundamental repeating block.

1. Space Lattice and Unit Cell

A. Crystal (Space) Lattice

A regular, infinitely repeating three-dimensional arrangement of points in space is called a crystal lattice.

  • Each point in a lattice is called a lattice point or lattice site.
  • Each lattice point represents one constituent particle (an atom, a molecule, or an ion).
  • Lattice points are joined by straight lines solely to bring out the geometry of the lattice.

B. The Unit Cell

The unit cell is the smallest portion (or building block) of a crystal lattice which, when repeated in different directions, generates the entire lattice.

Parameters of a Unit Cell:

  • Its dimensions along the three edges: a, b, and c.
  • The angles between these edges: $\alpha$ (between b and c), $\beta$ (between a and c), and $\gamma$ (between a and b).

2. The 7 Crystal Systems & 14 Bravais Lattices

French mathematician Auguste Bravais showed that there are only 14 possible three-dimensional lattices. These 14 Bravais Lattices are grouped into 7 Crystal Systems based on their edge lengths and axial angles.

⚠️ Memorizing this table is absolutely mandatory for JEE/NEET.

Crystal System Edge Lengths Axial Angles Possible Variations (Bravais Lattices) Classic Examples
1. Cubic $a = b = c$ $\alpha = \beta = \gamma = 90^\circ$ Primitive, Face-centered, Body-centered (3) $NaCl$, Zinc blende ($ZnS$), Copper, Diamond
2. Tetragonal $a = b \neq c$ $\alpha = \beta = \gamma = 90^\circ$ Primitive, Body-centered (2) White tin ($Sn$), $SnO_2$, $TiO_2$
3. Orthorhombic $a \neq b \neq c$ $\alpha = \beta = \gamma = 90^\circ$ Primitive, Face-centered, Body-centered, End-centered (4) Rhombic sulfur, $KNO_3$, $BaSO_4$
4. Hexagonal $a = b \neq c$ $\alpha = \beta = 90^\circ, \gamma = 120^\circ$ Primitive (1) Graphite, $ZnO$, $CdS$, Magnesium
5. Rhombohedral (Trigonal) $a = b = c$ $\alpha = \beta = \gamma \neq 90^\circ$ Primitive (1) Calcite ($CaCO_3$), Cinnabar ($HgS$)
6. Monoclinic $a \neq b \neq c$ $\alpha = \gamma = 90^\circ, \beta \neq 90^\circ$ Primitive, End-centered (2) Monoclinic sulfur, $Na_2SO_4 \cdot 10H_2O$
7. Triclinic $a \neq b \neq c$ $\alpha \neq \beta \neq \gamma \neq 90^\circ$ Primitive (1) Most Asymmetrical: $K_2Cr_2O_7$, $CuSO_4 \cdot 5H_2O$, $H_3BO_3$

3. The Cubic System: SC, BCC, and FCC

The cubic system is the most symmetrical ($a=b=c, \alpha=\beta=\gamma=90^\circ$) and the most heavily tested. We must calculate the Rank ($Z$) (effective number of atoms per unit cell), the relationship between edge length ($a$) and atomic radius ($r$), and the Packing Efficiency.

Atomic Contributions in a Cube:
  • An atom at the corner is shared by 8 adjacent cubes. Contribution = $1/8$.
  • An atom at the face-center is shared by 2 cubes. Contribution = $1/2$.
  • An atom at the body-center is inside the cube. Contribution = $1$.
  • An atom at the edge-center is shared by 4 cubes. Contribution = $1/4$.
1. Simple Cubic (SC)

Atoms are present only at the corners. Atoms touch each other along the edges.

  • Z: $8 \times (1/8) = \mathbf{1}$
  • Radius ($r$): $a = 2r \Rightarrow \mathbf{r = a/2}$
  • Coord. No: 6
  • Packing Eff: $\mathbf{52.4\%}$
2. Body-Centered (BCC)

Atoms at corners + 1 atom in the center of the body. Atoms touch along the body diagonal.

  • Z: $(8 \times 1/8) + 1 = \mathbf{2}$
  • Radius ($r$): $\sqrt{3}a = 4r \Rightarrow \mathbf{r = \frac{\sqrt{3}a}{4}}$
  • Coord. No: 8
  • Packing Eff: $\mathbf{68\%}$
3. Face-Centered (FCC)

Atoms at corners + 1 atom at the center of each face. Atoms touch along the face diagonal.

  • Z: $(8 \times \frac{1}{8}) + (6 \times \frac{1}{2}) = \mathbf{4}$
  • Radius ($r$): $\sqrt{2}a = 4r \Rightarrow \mathbf{r = \frac{a}{2\sqrt{2}}}$
  • Coord. No: 12
  • Packing Eff: $\mathbf{74\%}$ (Max)
Visualizing Cubic Unit Cells a = 2r Simple Cubic (SC) √3a = 4r Body-Centered (BCC) √2a = 4r Face-Centered (FCC)

The Density Formula

A guaranteed numerical question in exams relies on the density ($d$) formula for a cubic unit cell:

$d = \frac{Z \times M}{N_A \times a^3}$

Where:
$Z$ = Rank of unit cell (1 for SC, 2 for BCC, 4 for FCC)
$M$ = Molar mass of the substance (in g/mol)
$N_A$ = Avogadro's Number ($6.022 \times 10^{23} \text{ mol}^{-1}$)
$a^3$ = Volume of the unit cell (if $a$ is in cm, $d$ will be in $\text{g/cm}^3$)

Mastery Check: Unit Cells

15 High-Yield Questions to test your JEE/NEET Preparation

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